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Nuclear Fragmentation Reactions from Research to Applications

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Statistical Multifragmentation Model (SMM)<br />

J.P. Bondorf, R. Donangelo, I.N. Mishustin, et al., Nucl. Phys. A443 (1985) 321; A444 (1985) 460;<br />

J.P. Bondorf, A.S. Botvina, A.S. Iljinov, I.N. Mishustin, K. Sneppen, Phys. Rep. 257 (1995) 133<br />

α<br />

IMF<br />

n<br />

HR<br />

IMF<br />

p<br />

IMF<br />

Ensemble of nucleons and fragments<br />

in thermal equilibrium characterized by<br />

neutron number N0 pro<strong>to</strong>n number Z0 ,<br />

N0 +Z0 =A0 excitation energy E * =E0-ECN break-up volume V=(1+κ)V0 All break-up channels are enumerated by the sets of<br />

fragment multiplicities or partitions, f={NAZ },<br />

Total fragment multiplicity Mf = ∑AZNAZ Volume available for the translational motion, Vf (M),<br />

grows with the fragment multiplicity, approximately<br />

following P=const condition

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